
while for \(J^P=3/2^{-}\)  the Lagrangian contains a derivative \(\bar{D}^{*}\Xi _c\)  coupling [1]}
\(\mathcal {L}_{P_{c s} \Xi _{c} \bar{D}^{*}}&=-ig_{P_{c s}} \bar{P}_{c s}^{\mu }(x) \nonumber \\&\times \int dy\phi (y^2)\sum {}C_i\Xi _{c}(x+\omega _{\bar{D}^{*}}y)\bar{D}^{*} _{\mu }(x-\omega _{\Xi _c}y),\) 
